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基于量子自旋霍尔或谷霍尔效应的拓扑光子结构具有对缺陷免疫和抑制背向散射的特性, 对设计新型低损耗的光子器件起到了关键作用. 本文巧妙设计了一种具有时间反演对称性的二维电介质光子晶体, 实现了量子自旋霍尔效应和量子谷霍尔效应的共存. 首先基于蜂巢结构排布的硅柱经过收缩扩张, 打开了布里渊区
$ \varGamma $ 点的四重简并点形成拓扑平庸或非平庸的光子带隙, 实现量子自旋霍尔效应. 经过扩张后的蜂巢晶格演化成为Kagome结构, 之后在Kagome晶格中加入正负扰动, 打破光子晶体的空间反演对称性, 导致布里渊区的非等价谷$ K $ 和$ {K}' $ 的简并点打开并出现完整带隙, 实现了量子谷霍尔效应. 数值计算结果表明, 由拓扑平庸与非平庸、正扰动与负扰动的光子晶体组成的界面上可实现单向传输且对弯曲免疫的拓扑边缘态. 最后, 设计了基于两种效应共存的四通道系统, 此系统为光学编码与稳健信号传输提供潜在方法, 为电磁波的操纵提供了更大的灵活性.The location and transmission of light is the core of modern photonic integrated device, and the proposal of topological photonics provides a new way of implementing optical manipulation. Topological photonic structures based on the quantum spin hall effect or quantum valley hall effect have the properties of immunity to defects and suppress backscattering, so they play a key role in designing novel low-loss photonic devices. In this work, we design a two-dimensional dielectric photonic crystal with time-reversal symmetry to achieve the coexistence of the quantum spin hall effect and the quantum valley hall effect in a photonic crystal. The design can be likened to an electronic system in which two pairs of Kramers simplex pairs are constructed to achieve a quadruple simplex pair in a photonic crystal. First, based on the method of shrinking and expanding the silicon pillars arranged in the honeycomb structure, the quadruple degeneracy point at the Γ point of the first Brillouin zone is opened, and the corresponding topologically trivial or non-trivial photonic band gap is formed,thereby realizing quantum spin hall effect. The expanded honeycomb lattice evolves into a Kagome structure, and then positive and negative perturbations are added to the Kagome lattice, breaking the spatial inversion symmetry of the Photonic crystal. When mirror symmetry is broken, different chiral photonic crystals can be created,leading the degeneracy point of the non-equivalent valleys K and K' in the Brillouin zone to be opened and a complete band gap to appear, thus realizing the Quantum valley hall effect. In the common band gap, topologically protected edge states are induced by nontrivial valley Chern number at the interface between two photonic crystals with opposite chirality. The numerical calculations show that unidirectional transport and bending-immune topological boundary states can be realized at the interface composed of topologically trivial (non-trivial) and positively (negatively) perturbed photonic crystals. Finally, a four-channel system based on the coexistence of the two effects is designed, The system is a novel electromagnetic wave router that can be selectively controlled by pseudospin degree of freedom or valley degree of freedom. This system provides a potential method for realizing the optical encoding and robust signal transmission, thereby providing greater flexibility for manipulating electromagnetic waves.-
Keywords:
- photonic crystal /
- pseudospin /
- valley hall effect /
- topological phase transition
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图 1 PC示意图, 红色向量分别表示六边形和菱形原胞的单位向量, 长度
$ {a}_{0} $ 是晶格常数. 右图为六边形单胞的放大图, R为相邻硅柱间距, D为硅柱的直径,$ {\varepsilon }_{{\rm{d}}}{\rm{和}}{\varepsilon }_{{\rm{A}}} $ 分别是硅和周围环境的介电常数Fig. 1. PC schematic diagram, red vectors represent unit vectors of hexagonal and rhomboid unit cell respectively, and the length of lattice constant is
$ {a}_{0} $ . The right figure is an enlarged view of a hexagonal cell. R is the distance between adjacent silicon columns and D is the diameter of cylinder.$ {\varepsilon }_{{\rm{d}}}, {\varepsilon }_{{\rm{A}}} $ are dielectric constants of cylinder and surrounding environment, respectively.
图 2 (a)灰色区域表示菱形原胞的BZ, 用
$ Z $ 表示, 蓝色区域表示六边形原胞的BZ, 用$ {Z}_{{\rm{s}}} $ 表示, ($ {b}_{1}, {b}_{2} $ )和($ {b}_{{\rm{s}}1}, {b}_{{\rm{s}}2} $ )是对应的倒格子基矢; (b)从$ Z $ 到$ {Z}_{{\rm{s}}} $ 的折叠机制示意图; (c)菱形原胞的BZ内选择不同的扫描路径的能带色散图及折叠到六边形原胞的BZ内的能带色散图; (d)基于单胞$ {C}_{{\rm{s}}} $ 的色散曲线, 插图为原始单胞和扫描的BZ, 结构参数为${a}_{0}=1~{\rm{μ }}{\rm{m}}$ ,$D=0.24 {a}_{0}$ ,$ R/{a}_{0}=1/3 $ , 右图为狄拉克四重简并点的电场图Fig. 2. (a) The gray area denoted by
$ Z $ represents the BZ of the rhomboid unit cell; the blue area denoted by$ {Z}_{{\rm{s}}} $ represents the BZ of the hexagonal unit cell; ($ {b}_{1}, {b}_{2} $ ) and ($ {b}_{{\rm{s}}1}, {b}_{{\rm{s}}2} $ ) are the corresponding inverted lattice basis vectors, respectively; (b) the folding mechanism from$ Z $ to$ {Z}_{{\rm{s}}} $ ; (c) band dispersion maps in the BZ of the rhomboid unit cell with different scanning paths, and band dispersion maps with different scanning paths based on the folding mechanism; (d) dispersion curves based on a single cell$ {C}_{{\rm{s}}} $ , and the inset is the original single cell and the scanned BZ, the structural parameters are${a}_{0}=1~{\rm{μ }}{\rm{m}}$ ,$D=0.24 {a}_{0}$ ,$ R/{a}_{0}=1/3 $ , the right of Fig. (d) is electric fields of Dirac quadruple degenerate points.
图 3
$ R/{a}_{0}=0.25 $ ($D=0.36 {a}_{0}$ ) (a)和$ R/{a}_{0}=0.5 $ ($D=0.4 {a}_{0}$ )(b)的能带图, 说明$ \varGamma $ 发生p, d模式反转(b); (c)晶格结构为$ R/{a}_{0}=0.25 $ 时上下能级的电场图(左1和左2)和晶格结构为$ R/{a}_{0}=0.5 $ 时上下能级的电场图(右1和右2)Fig. 3. Energy bands of lattices with
$ R/{a}_{0}=0.25 $ ($D=0.36 {a}_{0}$ )(a) and$ R/{a}_{0}=0.5 $ ($D=0.4 {a}_{0}$ )(b), respectively, the p and d modes reversal occurs in$ \varGamma $ (b); (c) two columns on the left: electric fields of the p or d state at point Γ for the lattice with$R/{a}_{0}=0.25\left({\rm{l}}{\rm{e}}{\rm{f}}{\rm{t}}\; 1\;{\rm{ }}{\rm{a}}{\rm{n}}{\rm{d}}\;2\right)$ , two columns on the right: electric fields for the p or d state for the lattice with$R/{a}_{0}=0.5\left({\rm{r}}{\rm{i}}{\rm{g}}{\rm{h}}{\rm{t}}{\rm{ }}\;1\;{\rm{ }}{\rm{a}}{\rm{n}}{\rm{d}}\; 2\right)$ 
图 4 (a)KPC的结构示意图; (b)
$D=0.4 {a}_{0}, R/{a}_{0}=0.5, d=1.2 {d}_{0}$ 或$d=0.8 {d}_{0}~({d}_{0}=\dfrac{{a}_{0}}{2 \sqrt{3}})$ 的KPC的色散曲线; (c)第一、二条能带$K\left({K}'\right)$ 点的相位图及上下能带$ \varGamma $ 点的电场图; (d)KPC原胞正扰动和负扰动第一条能带的Berry曲率Fig. 4. (a) The structure diagram of KPC; (b) the dispersion curve of KPC with
$D=0.4 {a}_{0}$ ,$ R/{a}_{0}=0.5 $ ,$d=1.2 {d}_{0}$ or$d=0.8 {d}_{0} $ $ \Big({d}_{0}=\dfrac{{a}_{0}}{2\sqrt{3}}\Big)$ ; (c) phase diagram of the first and second band$K\left({K}'\right)$ and electric field diagram of the upper and lower band$ \varGamma $ ; (d) Berry curvature of the first band of positive or negative perturbations of the KPC unit cell.
图 5 (a)赝自旋极化边缘态, 拓扑平凡PC和拓扑非平凡PC组成超胞的几何结构、能带结构以及A, B两点对应的电场分布图;(b)谷极化边缘态, 由正扰动和负扰动KPC结构所组成的几何结构、能带结构以及A, B两点对应的电场分布图
Fig. 5. (a) Pseudospin-polarized edge states, the structure and the energy band of a supercell composed of the topological trivial PC and the topological nontrivial PC, and the electric field distribution corresponding to points A and B at the energy band; (b) valley-polarized edge states, the geometry and band structure of the KPC consisting of positive and negative perturbations and the corresponding electric field distribution at points A and B.
图 6 赝自旋边缘态的光传输特性和场分布(a)由
$ R=0.5*{a}_{0} $ (蓝色区域)非平凡结构和$ R=0.25*{a}_{0} $ 平凡结构(红色区域)组成直波导示意图, 图中黄色的六角形表示手性源的位置; (b)6个点源组成的手性激发源示意图, 相邻点源的相位差是$ {\text{π}}/3 $ ; (c)和(d)直波导中分别由RCP和LCP光源所激发的光束电场强度分布; (e)由$ R=0.5*{a}_{0} $ (蓝色区域)和$ R=0.25*{a}_{0} $ (红色区域)组成的“Z”字形波导; (f)Z字形波导中RCP源所激发的电场分布图Fig. 6. Optical transmission characteristics and the electric field distribution of the pseudospin boundary state: (a) Schematic diagram of the straight waveguide consisting of the non-trivial structure with
$ R=0.5*{a}_{0} $ (blue area) and the trivial structure with$ R=0.25*{a}_{0} $ (red area), the yellow hexagon in the diagram shows the position of the excitation source; (b) schematic diagram of a chiral power consisting of six antennas, and the phase difference between adjacent antennas is π/3; (c), (d) the electric field intensity distributions excited by RCP or LCP sources, respectively; (e) Z-shaped waveguide consisting of$ R=0.5*{a}_{0} $ (blue area) and$ R=0.25*{a}_{0} $ (red area); (f) field intensity distribution of the electric field excited by the RCP source.
图 7 谷边缘态的光传输特性和场分布(a)由
$d = 0.8{d}_{0}$ (蓝色区域)和$d = 1.2{d}_{0}$ (红色区域)组成的直波导示意图, 左手性源(标记为六角形)放置在正扰动和负扰动KPC界面附近的不同位置处, 以激发不同的边缘模式; (b)—(d)分别由LCP光源在不同的激发源位置所激发的光束电场强度分布; (e)和(f)分别是构建的“Z”字形拓扑波导, 以及由黄星表示的LCP源所激发的电场强度分布Fig. 7. Optical transmission characteristics and the electric field distribution of the valley edge state: (a) Schematic diagram of valley waveguide composed of
$d=0.8 {d}_{0}$ (blue region) and$d=1.2 {d}_{0}$ (red region), the left-handed circular polarized dipoles (marked as the hexagon) placed at different locations near the interface between KPCs with positive or negative disturbances to excite edge modes; (b)–(d) are the electric field intensity distributions excited by the LCP light source at different positions; (e) schemes of z-shaped waveguide; (f) the electric field intensity distribution of Z-shaped waveguide excited by the LCP source. -
[1] Klitzing V K 2017 Annu. Rev. Conden. Ma. P. 8 13
Google Scholar
[2] Qi X L, Zhang S C 2011 Rev. Mod. Phys. 83 1057
Google Scholar
[3] Haldane F D, Raghu S 2008 Phys. Rev. Lett. 100 013904
Google Scholar
[4] Wang Z, Chong Y D, Joannopoulos J D, Soljačić M 2009 Nature 461 772
Google Scholar
[5] 沈清玮 徐林 蒋建华 2017 物理学报 66 224102
Google Scholar
Shen Q W, Xu L, Jiang J H 2017 Acta Phys. Sin. 66 224102
Google Scholar
[6] Khanikaev A B, Hossein Mousavi S, Tse W K, Kargarian M, MacDonald A H, Shvets G 2013 Nat. Mater. 12 233
Google Scholar
[7] Chen W J, Jiang S J, Chen X D, Zhu B, Zhou L, Dong J W, Chan C T 2014 Nat. Commun. 5 1
[8] He C, Sun X C, Liu X P, Lu M H, Chen Y, Feng L, Chen Y F 2016 Proc. Natl. Acad. Sci. U. S. A. 113 4924
Google Scholar
[9] Hafezi M, Demler E A, Lukin M D, Taylor J M 2011 Nat. Phys. 7 907
Google Scholar
[10] Hafezi M, Mittal S, Fan J, Migdall A, Taylor J M 2013 Nat. Photonics 7 1001
Google Scholar
[11] Chen W J, Jiang S J, Chen X D, Zhu B, Zhou L, Dong J W, Chan C T 2014 Nat. Commun. 5 5782
Google Scholar
[12] Liang G Q, Chong Y D 2013 Phys. Rev. Lett. 110 203904
Google Scholar
[13] Ma T, Khanikaev A B, Mousavi S H, Shvets G 2015 Phys. Rev. Lett. 114 127401
Google Scholar
[14] Wu L H, Hu X 2015 Phys. Rev. Lett. 114 223901
Google Scholar
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Google Scholar
[16] Anderson P D, Subramania G 2017 Opt. Express 25 23293
Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
Fang Y T, Wang Z X, Fan E P, Li X X, Wang H J 2020 Acta Phys. Sin. 69 184101
Google Scholar
[22] 王彦兰, 李妍 2020 物理学报 69 094206
Google Scholar
Wang Y L, Li Y 2020 Acta Phys. Sin. 69 094206
Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
[31] He X T, Liang E T, Yuan J J, Qiu H Y, Chen X D, Zhao F L, Dong J W 2019 Nat. Commun. 10 1
Google Scholar
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Google Scholar
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Google Scholar
[34] Zhong H, Li Y D, Song D H, Kartashov Y V, Zhang Y Q 2020 Laser Photonics Rev. 14 7
[35] Zhong H, Xia S Q, Zhang Y Q, Li Y D, Song D H, Liu C L, Chen Z G 2021 Adv. Photonics 3 056001
[36] Tang Q, Zhang Y Q, V. Kartashov Y, Li Y D, V. Konotop V 2022 Chaos Solitons Fractals 161 112364
Google Scholar
[37] Tang Q, Ren B Q, Belić M R, Zhang Y Q, Li Y D 2022 Rom. Rep. Phys. 74 405
[38] Ren B Q, Wang H G, O. Kompanets V, V. Kartashov Y, Li Y D, Zhang Y Q 2021 Nanophoton. 10 3559
Google Scholar
[39] Arora S, Bauer T, Barczyk R, Verhagen E, Kuipers L 2021 Light Sci. Appl. 10 1
Google Scholar
[40] Chen M L, Jiang L J, Lan Z H, Sha W 2020 Phys. Rev. Res. 2 043148
Google Scholar
[41] Wei G C, Liu Z Z, Wang L C, Song J Y, Xiao J J 2022 Photonics Res. 10 999
Google Scholar
[42] Wu L H, Hu X 2016 Sci. Rep. 6 1
Google Scholar
[43] Liu F, Deng H Y, Wakabayashi K 2019 Phys. Rev. Lett. 122 086804
Google Scholar
[44] Wang C, Zhang H, Yuan H, Zhong J, Lu C 2020 Front. Optoelectron. 13 73
Google Scholar
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